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Higgs Boson Studies at the Tevatron in Run II
Thomas R. Junk Fermilab
On Behalf of the CDF and D0 Collabora;ons
APS April Mee;ng, Denver, CO April 14, 2013
T. Junk Tevatron Higgs Results
• The Tevatron, CDF, and D0 • Higgs Boson Produc;on and Decay • Highlights of Search Techniques – What we Learned • Results: Limits, Cross Sec;ons, Significance • Results: Couplings, BSM models
4/14/13
T. Junk Tevatron Higgs Results 2
Fermilab from the Air
CDF D0
Chicago→
Main Injector – new for Run II pbar recycler – not used to recycle pbars but used as a second storage ring to accumulate pbars
Tevatron
!
pp Collisions at s =1.96 TeV
pbar accumulator
1 km
4/14/13
4/14/13 T. Junk Tevatron Higgs Results T. Junk Tevatron Measmnts and Disc. 3
The Tevatron, Like All Accelerators, Improved in Performance Over Time
Total delivered luminosity: ~12 W-‐1 each to CDF and D0. Acquired and analyzed: ~10 W-‐1 each.
Many thanks to the Fermilab Beams Division!
T. Junk Tevatron Higgs Results
First CDF pp event: 1985 End of opera;ons: 2011
Lepton coverage: |η| < 1.5 (muons) |η| < 2.0 (electrons) b-‐tagging with |η| < ~1.4 Jets to |η| < 2.8 Higgs analyses restrict to |η| < 2.0 Dijet mass resoluMon: ~16%
4/14/13
T. Junk Tevatron Higgs Results
The Detector
New Innermost Silicon Layer added between Run IIa and Run IIb
Lepton coverage: |η| < 2 (muons) |η| < 2.6 (electrons) b-‐tagging with |η| < ~2 Jets to |η| < 3
Similar dijet mass resolu;on to CDF
Scin;lla;ng fiber tracker Trigger similar to CDF’s
Good Feature: Regular Switching of Solenoid Field – Cancels Some Systema;c Uncertain;es
4/14/13
1
10
10 2
10 3
100 125 150 175 200 225 250 275 300mH [GeV]
(pp
H+X
) [fb]
Tevatrons=1.96 TeV
pp–H (NNLO+NNLL QCD + NLO EW)
pp–
WH (NNLO QCD + NLO EW)
pp–ZH (NNLO QCD + NLO EW)
pp– qqH (NNLO QCD + NLO EW)pp–tt–H (NLO QCD)
[GeV]HM100 200 300 400 500 1000
Higg
s BR
+ T
otal
Unc
ert
-310
-210
-110
1
LHC
HIG
GS
XS W
G 2
011
bb
cc
ttgg
Z
WW
ZZ
SM Higgs Boson Production and Decay Rates
Primary analysis modes: mH<130 GeV: VHàVbb mH>130 GeV: ggàHàWW
Addi;onal modes: Hàττ, Hàγγ, HàZZà4l
Gluon Fusion
Associated Produc;on
Vector Boson Fusion
t
t iH
T. Junk Tevatron Higgs Results 4/14/13
T. Junk Tevatron Higgs Results
Tevatron Hàbb Publications, Summer 2012
CDF, D0, and Tevatron Publica;ons: CDF lvbb: Phys. Rev. Lei. 109, 111804 (2012) Includes new HOBIT b-‐tagger CDF llbb: Phys. Rev. Lei. 109, 111803 (2012) Includes new HOBIT b-‐tagger CDF METbb: Phys. Rev. Lei. 109, 111805 (2012) Uses old SECVTX+JetProb b-‐taggers CDF Combined Hàbb: Phys. Rev. Lei. 109, 111802 (2012) D0 lvbb: Phys. Rev. Lei. 109, 121804 (2012) D0 llbb: Phys. Rev. Lei. 109, 121803 (2012) D0 METbb: Phys. Lei. B 716, 285 (2012) D0 Combined Hàbb: Phys. Rev. Lei. 109, 121802 (2012) Tevatron Combined Hàbb: Phys. Rev. Lei. 109, 071804 (2012)
4/14/13
T. Junk Tevatron Higgs Results
Associated production VH
H
b
b!
l-
l
Jet
Jet
ν
l
ν
ν!
1)
2)
3)
V
Friday, November 9, 12
“lvbb”
“METbb” or “vvbb”
“llbb”
Drawing Credit: CMS Higgs TWiki. CDF also seeks qqHàqqbb and iHàibb
The Main Associated Production Search Channels
4/14/13
T. Junk Tevatron Higgs Results
Tevatron Hàbb Results, Summer 2012
Maximum local significance: 3.3σ at mH=135 GeV/c2 Global significance: 3.1σ – Evidence for VHàVbb. Local significance at mH=125 GeV/c2 is 2.8σ
Cross sec;on fit at mH=125 GeV/c2
(!WH +! ZH )!B(H" bb ) = 0.23#0.080+0.090 (stat+syst) pb
SM Predic;on: 0.12 ± 0.01 pb
Phys. Rev. Lei. 109, 071804 (2012)
4/14/13
Status from the LHC
A Higgs-‐like parMcle is firmly established, its mass looks to be between 125 and 126 GeV, and its properMes are consistent with the SM Higgs boson
Many more superb results are available at hips://twiki.cern.ch/twiki/bin/view/AtlasPublic/HiggsPublicResults hips://twiki.cern.ch/twiki/bin/view/CMSPublic/PhysicsResultsHIG
T. Junk Tevatron Higgs Results
(as of HCP 2012)
4/14/13
T. Junk Tevatron Higgs Results
Recent Publications Contributing to the Final Higgs Combination
CDF: METbb: Phys. Rev. D 87, 052008 (2013). HWWàlvlv: PRD in prepara;on. FERMILAB-‐PUB-‐13-‐029-‐E All Hadronic final state: JHEP 1302, 004 (2013) iHàibb: Phys. Rev. Lei 109, 181802 (2012). SM/SM4/FP/Coupling Combina;on: arXiv:1301.6668 (2013). Submiied to Phys. Rev. D
D0: H/WH/ZHàleptons+tau+jets: arXiv:1211.6993. Accepted by Phys. Rev. D WH/ZH Trileptons and same-‐sign dileptons: arXiv:1302.5723 Submiied to Phys. Rev. D H/WH/ZHàlvbb+lvjj + lvjjjj: arXiv:1301.6122 Accepted by Phys. Rev. D HàDiphotons: arXiv:1301.5358 Accepted by Phys. Rev. D HàWWàlvlv: arXiv:1301.1243 Accepted by PRD SM/SM4/FP Combina;on: arXiv:1303.0823 Submiied to Phys. Rev. D
Tevatron Combina;on Manuscript: arXiv:1303.6346 Submiied to Phys. Rev. D
4/14/13
All CDF SM Search Channels
T. Junk Tevatron Higgs Results 4/14/13
T. Junk Tevatron Higgs Results
All D0 SM Search Channels
4/14/13
T. Junk Tevatron Higgs Results 14
B-‐Tagging
Mistag rates typically ~1% for light-flavor jets
Example candidate event (lvbb)
Impact parameter resolution for high-pT tracks ~18µm
L00 single-sided silicon + 5-layer double-sided silicon+ 2-layer ISL
B-‐tagging relies on displaced vertex reconstruc;on: high mass, long life;me
D0: Boosted Decision Treetagging algorithm. Per-jetefficiency = 50-70% (of taggablejets) for 1-5% Mistag rate
4/14/13
T. Junk Tevatron Higgs Results
CDF’s HOBIT b-tagger – Improved Sensitivity With Respect to the SECVTX, Roma, and BNess taggers
HOBIT Tight and Loose opera;ng points chosen to have similar mistag rates as older SECVTX opera;ng points. More signal More b background Similar LF background
A neural-‐network b-‐tagger using inputs from other b-‐taggers, as well as lepton ID to include semileptonically decaying B hadrons.
J. Freeman et al., Nucl. Instrum. Methods A 697, 64 (2012). see also M. Stancari, Fermilab Joint Experimental/Theore;cal Seminar, Mar. 7 2012
OperaMng Point
Mistag rate
SECVTX efficiency
HOBIT efficiency
Tight 1.4% 39% 54%
Loose 2.9% 47% 59%
per-‐jet efficiencies shown
4/14/13
T. Junk Tevatron Higgs Results
q
q’
W* W
l
ν
H0 b
b
D0 Collab., PRL 109, 121804 (2012); D0 Collab., arXiv:1301.6122 [hep-‐ex]; CDF Collab., PRL 109, 111804 (2012)
Associated Production of a Higgs Boson with a W Boson
Double Tight Tag yields (D0) Expected signal: 17.3±1.7 events of WH (mH=125 GeV) 1.9±0.1 events of ZH (mH=125 GeV) Expected Background: 10404±1059 events Data 10071 events Expected limit @125: 4.7*SM (2.8*SM for CDF)
Dijet mass resolu;on: 13% to 23% depending on the number of jets and tags. 3-‐jet events or 1-‐tag events: more likely to misassign an ISR/FSR jet to the Higgs decay
4/14/13
T. Junk Tevatron Higgs Results
q
q
Z0* Z0
ν
ν
H0 b
b
Double Tight Tag yields (CDF) Signal (ZH) 1.9±0.3 events (mH=125 GeV) Background: 131±26 events Data: 117 Events Expected limit @125: 3.9*SM CDF, (5.1*SM for D0)
CDF Collab., PRL 109, 11803 (2012) D0 Collab., PRL 109, 121803 (2012)
ZHàllbb: A Fully Reconstructed Channel
125 GeV Final Discriminat 0 0.5 1
Even
ts/B
in
-210
-110
1
10
210 data Z+lf Z+bb Z+cc WW WZ ZZ tt fake ZZH(125)x10
+ Two Jets, Two Tight b-Tags -µ+µ
-1CDF Run II Prelimary 9.45 fbVery innova;ve channel! • Loose lepton ID. Tag and probe lepton ID efficiency calibra;on in data • Split into 2 jet, 3 jet, single, double, ;ght, and loose b-‐tags • NN dijet mass using MET projec;ons • Cascade of neural networks: Train networks to separate ibar, Diboson, Wbb backgrounds from signal.
Excellent reconstruc;on countered by low Zàll branching ra;o
“Raw” dijet mass
Dijet mass a}er NN Correc;on 12% resol. in some channels
4/14/13
T. Junk Tevatron Higgs Results
CDF Collab., PRL 109, 111805 (2012) Updated with HOBIT: PRD 87, 052008 (2013) D0 Collab., Phys. Lei. B 716, 285 (2012)
VHàMETbb Analysis
Cascade of neural networks: First an;-‐QCD, second Higgs vs. remaining backgrounds
Double-‐;ght tags, CDF yields: Signal (WH125): 5.3±0.5 Signal (ZH125): 5.4±0.5 Background: 759±86 Data: 692 Expected limit: 3.3*SM (3.9*SM for D0)
4/14/13
T. Junk Tevatron Higgs Results
HàWW Searches
D0 Collab., PRD 86, 032010 (2012) CDF Collab., FERMILAB-‐PUB-‐13-‐029-‐E (in prepara;on)
W-
W+ e+
e-
ν
ν
Largest signal is from gluon fusion, but WH, ZH, and VBF contribute as well.
Dominant background at the Tevatron is nonresonant WW produc;on
ΔRll tends to be smaller in signal events than for background events
But we split the samples into lvlv + 0j lvlv + 1j lvlv + 2 or more jets and the backgrounds vary by subsample.
H0
4/14/13
T. Junk Tevatron Higgs Results
0-jet DY-BDT-1 -0.6 -0.2 0.2 0.6 1
Even
ts/0
.10
-210
-1101
10
210
310
410
510
610
710
810 DataSignalZ+jetsDibosonW+jetsMultijettt
Bkg. syst.
TE, ee + -1DØ, 9.7 fb
Signature: Two oppositely-‐signed leptons, large missing ET. Low ΔΦll, low ΔRll Large DY background in ee and μμ channels, not so much in eμ. DY has low missing ET, mll near mZ, and other characteris;cs. Recent improvements: • Looser lepton ID • low-‐mll channel, • modify isola;on requirement so leptons don’t spoil each other’s isola;on. • Split channels into more categories: Data calibra;on of lepton ID efficiency for new loose lepton categories. Control regions to validate backgrounds: DY, WW, Wγ, W+jets, ibar
HàWW Searches
DY BDT removes most of DY(+jets)
0-jet WW-depleted Final BDT0 0.2 0.4 0.6 0.8 1
Even
ts/0
.04
-110
1
10
210
310
410DataSignalZ+jetsDibosonW+jetsMultijettt
Bkg. syst.
TE, ee + -1DØ, 9.7 fb
0-jet WW-enriched Final BDT0 0.2 0.4 0.6 0.8 1
Even
ts/0
.04
-110
1
10
210
310
410 DataSignalZ+jetsDibosonW+jetsMultijettt
Bkg. syst.
TE, ee + -1DØ, 9.7 fb
WW-‐enriched WW-‐depleted
D0 Collab., arXiv:1301.1243 [hep-‐ex]
4/14/13
T. Junk Tevatron Higgs Results
Validation of HàWW Analysis by Measuring the WW Cross Section
Cross Section (pb)
TE, ll + -1DØ, 9.7 fb
5 10 15 20 25 30
eeWW 1.1 (syst)± 1.1 (stat) ±13.3
µµWW 0.7 (syst)± 0.9 (stat) ±11.5
µeWW 0.6 (syst)± 0.6 (stat) ±11.1
combinedWW 0.6 (syst)± 0.4 (stat) ±11.6
NLOWW 0.7±11.3
Campbell and Ellis, PRD 60, 113006 (1999)
(s/b)10
log-3 -2.5 -2 -1.5 -1 -0.5 0 0.5 1 1.5
Even
ts
0
100
200
300
400 Data - BkgdSignal (WW)1 s.d. on Bkgd±
TE, ll + -1DØ, 9.7 fb
Same Selec;on, Similar MVA’s Measure WW cross sec;on of (1.02±0.06)*SM(MCFM v6.0)
D0 Collab., arXiv:1301.1243 [hep-‐ex]
4/14/13
T. Junk Tevatron Higgs Results
1
10
0 2 4 6 8 10 12 14Integrated Luminosity (fb-1)
Expe
cted
Lim
it/SM Summer 2005
Summer 2006Summer 2007Winter 2008Fall 2008
Fall 2009Summer 2010Summer 2011Winter 2012
mH=115 GeV/c2
SM=1
1
10
0 2 4 6 8 10 12 14Integrated Luminosity (fb-1)
Expe
cted
Lim
it/SM Summer 2004
Summer 2005Summer 2007Winter 2008Fall 2008
Spring 2009Fall 2009Summer 2010Summer 2011Winter 2012
mH=160 GeV/c2
SM=1
Sensitivity Evolution over Time
We collected data, and we also learned how to get more out of the data. • Beier MVA’s • Beier Event Selec;on • Beier lepton ID • Beier jet energy resolu;on • More triggers • More analysis categories • Sharing improvements between analyses
CDF sensi;vi;es shown. D0’s sensi;vi;es are similar
4/14/13
Tevatron Diboson Search in the Higgs Analyses
! (WZ + ZZ ) = 4.4± 0.3 pb
SM Predic;on:
Measurement:
! (WZ + ZZ ) = 3.0± 0.6 pb
A look at the summed mjj distribu;on
T. Junk Tevatron Higgs Results
)2Dijet Mass (GeV/c0 50 100 150 200 250 300 350 400
) 2Ev
ents
/ (2
0 G
eV/c
0
200
400
600
800
Data - BkgdWZZZHiggs Signal
2=125 GeV/cHm
-1 10 fb intTevatron Run II, L1+2 b-Tagged Jets
)2Dijet Mass (GeV/c0 50 100 150 200 250 300 350 400
) 2Ev
ents
/ (1
0 G
eV/c
0
2000
4000
6000
8000
10000
DataWZZZBkgd
-1 10 fb intTevatron Run II, L1+2 b-Tagged Jets
Check of the VHàVbb channels using the WZ+ZZ signal as a standard candle
4/14/13
SM Combined Data Summary at mH=125 GeV/c2
Background Hypothesis fit to data Bins of similar s/b added together Data error bars are sqrt(nobs)
T. Junk Tevatron Higgs Results
10-4
10-3
10-2
10-1
1
10
10 2
10 3
10 4
10 5
10 6
-4 -3 -2 -1 0log10(s/b)
Even
ts/0
.16
DataBackground fitSM Higgs signal
mH=125 GeV/c2
Tevatron Run II, Lint 10 fb-1
SM Higgs combination
4/14/13
SM Combined Data Summary at mH=125 GeV/c2
Same as before, but fiied background subtracted from the data. Data error bars are sqrt(s+bfit)
T. Junk Tevatron Higgs Results
-250
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-3 -2.5 -2 -1.5 -1 -0.5 0log10(s/b)
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ts/0
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Data-background
SM Higgs signal
±1 s.d. on background
Tevatron Run II, Lint 10 fb-1
SM Higgs combination
mH=125 GeV/c2log10(s/b)
Even
ts/0
.25
-10
-5
0
5
10
-1 -0.75 -0.5 -0.25 0
4/14/13
T. Junk Tevatron Higgs Results
)2 (GeV/cHm100 120 140 160 180 200
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lihoo
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atio
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-10
0
10
20
30
40 1 s.d.± bLLR 2 s.d.± bLLR
bLLRs+bLLRObsLLR
)2=125 GeV/cH
1.0 (m× H)2=125 GeV/c
H 1.5 (m× H
-1 10 fb intTevatron Run II, LSM Higgs Combination
Tevatron Combined SM LLR Distributions
LLR is a ra;o of the compa;bility of the data with the signal+background hypothesis and the background-‐only hypothesis. Data show a clear preference for a Higgs boson with mH between 115 and 140 GeV 4/14/13
T. Junk Tevatron Higgs Results
)2 (GeV/cHm100 120 140 160 180 200
Log-
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bLLRs+bLLRObsLLR
)2=125 GeV/cH
1.0 (m× H)2=125 GeV/c
H 1.5 (m× H
-1 10 fb intTevatron Run II, LSM Higgs Combination
August 2006
March 2013: Final
Tevatron Combined LLR Over the Years
Dec. 2007 Apr. 2008
4/14/13
Tevatron Final SM Higgs Rate and Mass Limits
Excluded regions: 90 < mH < 109 GeV/c2 and 149 < mH < 182 GeV/c2 Expect to exclude if no Higgs: 90 < mH < 120 GeV/c2 and 140 < mH < 184 GeV/c2
T. Junk Tevatron Higgs Results
1
10
100 120 140 160 180 200
1
10
mH (GeV/c2)
95%
C.L
. Lim
it/SM Tevatron Run II, Lint 10 fb-1
SM Higgs combinationObservedExpected w/o HiggsExpected ±1 s.d.Expected ±2 s.d.Expected if mH=125 GeV/c2
SM=1
4/14/13
Tevatron Combined SM Higgs Boson Search p-value
Observed local significance at mH=125 GeV/c2 is 3.1σ Expected significance assuming mH=125 GeV/c2 is shown with a doied line (not quite 2σ)
Look-‐Elsewhere Effect: • mH~125 GeV has been firmly established by the LHC • CDF+D0’s mass resolu;on is not very sharp -‐-‐ ~2 independent search results in Hàbb, ~2 in HàWW • Technical challenge – MVA’s trained at each mH separately. Histograms of predic;ons exchanged. Would need to exchange correlated pseudoexperiments to compute LEE exactly.
T. Junk Tevatron Higgs Results
)2 (GeV/cHm100 120 140 160 180 200
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grou
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ue
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ObservedExpected w/ Higgs
1 s.d.±Expected 2 s.d.±Expected )2=125 GeV/c
H 1.0 (m× H
)2=125 GeV/cH
1.5 (m× H
-1 10 fb intTevatron Run II, LSM Higgs Combination
4/14/13
Best-Fit Tevatron Combined Cross Sections at mH=125 GeV/c2
H! !! : 5.97"3.12+3.39 #SMH!W +W " : 0.94"0.83
+0.85 #SM
H! ! +! " : 1.68"1.68+2.28 #SMVH!Vbb : 1.59"0.72
+0.69 #SM
Combined : 1.44!0.56+0.59 "SM
T. Junk Tevatron Higgs Results
Br)/SM× Best Fit (0 1 2 3 4 5 6 7 8 9 10
b VbVH
-+ H
-W+ WH
H
2 = 125 GeV/cHm
Combined (68% C.L.)
Single channel
-1 10 fb intTevatron Run II, L
0
0.5
1
1.5
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2.5
3
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1
1.5
2
2.5
3
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mH (GeV/c2)/S
M
SM=1
Tevatron Run II, Lint 10 fb-1 SM Higgs combination
±1 s.d.±2 s.d.
ObservedH x 1.5 (mH=125 GeV/c2)H x 1.0 (mH=125 GeV/c2)
4/14/13
Final Tevatron Combined VHàVbb Cross Section Measurements
The SM predic;on is
! (WH + ZH )!Br(H" bb ) = 0.120± 0.008 fb
At mH=125 GeV/c2, the measured rate is
! (WH + ZH )!Br(H" bb ) = 0.19#0.09+0.08 pb
arXiv:1303.6346
T. Junk Tevatron Higgs Results
! (WH + ZH )!Br(H" bb ) = 0.23#0.08+0.09 pb
at mH=125 GeV/c2
Phys. Rev. Lei. 109, 071804 (2012)
0
100
200
300
400
500
600
90 100 110 120 130 140 1500
100
200
300
400
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600
mH (GeV/c2)
(W
H+
ZH) x
Br(H
bb– ) (fb
)
Tevatron Run II, Lint 10 fb-1
SM H bb– combinationMeasured±1 s.d.±2 s.d.Predicted
H x 1.5 (mH=125 GeV/c2)
H x 1.0 (mH=125 GeV/c2)
The change is due to CDF’s updated METbb channel
4/14/13
T. Junk Tevatron Higgs Results
)2 (GeV/cHm100 110 120 130 140 150 160 170 180 190 200
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H 1.5 (m× H
-1 10 fb intTevatron Run II, LWW CombinationSM H
)2 (GeV/cHm100 105 110 115 120 125 130 135 140
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H 1.5 (m× H
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Tevatron Combined HàWW Searches
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Br(H
WW
))/SM
SM=1
Tevatron Run II, Lint 10 fb-1
SM H W+W- combination ±1 s.d.±2 s.d.
Observed
H x 1.5(mH=125 GeV/c2)
H x 1.0(mH=125 GeV/c2)
4/14/13
Zoom-‐in at lower masses:
T. Junk Tevatron Higgs Results
1
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10 2
100 105 110 115 120 125 130 135 140 145 150
1
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mH (GeV/c2)95
% C
.L. L
imit/
SM Tevatron Run II, Lint 10 fb-1
SM H combination
SM=1
Expected w/o Higgs
Observed
Expected ±1 s.d.
Expected ±2 s.d.
1
10
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100 105 110 115 120 125 130 135 140 145 150
1
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mH (GeV/c2)
95%
C.L
. Lim
it/SM Tevatron Run II, Lint 10 fb-1
SM H + - combination
SM=1
Expected w/o Higgs
Observed
Expected ±1 s.d.
Expected ±2 s.d.
Tevatron Combined Hàτ+τ- and Hàγγ Searches
A bit of an excess (2σ at mH=125 GeV) seen in Hàγγ
4/14/13
Extensions to the SM: Fourth-Generation Models (SM4)
A heavy fourth genera;on of quarks would scale the gg→H produc;on rate at colliders by a factor of ~9. But watch out for H→ν4ν4 decays. E. Arik et al., Acta Phys. Polon. B 37, 2839 (hep-‐ph/0502050)
Kribs, Spannowsky, Plehn, Tait, Phys. Rev. D 76, 075016 (2007) T. Junk Tevatron Higgs Results 4/14/13
Searches for ggàHàWW – Model Independent and SM4 interpretation
SM4 Cross Sec;ons computed at NNLO in QCD by Anastasiou, Boughezal, and Furlan, JHEP 1006, 101 (2010)
Searches op;mized specifically for ggàH (NN’s not trained with WH, ZH, or VBF). Limit on cross sec;on ;mes b.r. shown along with SM4 model predic;ons.
Low-‐Mass scenario: ml4=100 GeV, mv4=80 GeV High-‐Mass scenario: ml4=mv4=1 TeV Both Scenarios: md4=400 GeV, mu4=450 GeV Note: mv4 lower bound is from L3’s unstable 4th genera;on neutrino search. P. Achard et al., PLB 517, 75 (2001). A stable v4 could be lighter. K. Belotsky et al., PRD 68, 054027 (2003).
Low-‐mass scenario exclusions: Expected exclusion: 118 < mH < 270 GeV/c2 Observed exclusion: 121 < mH < 225 GeV/c2
T. Junk Tevatron Higgs Results
10-1
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H)×
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Tevatron Run II, Lint 10 fb-1
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Exp. 95% C.L. LimitObs. 95% C.L. Limit±1 s.d. Exp. Limit±2 s.d. Exp. LimitSM4 (low mass)SM4 (high mass)
(w/o Higgs)
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. Lim
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ass)
Pre
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ion
Tevatron Run II, Lint 10 fb-1
SM4 Higgs combination
SM4(low mass)=1
Expected w/o HiggsObserved±1 s.d. Expected±2 s.d. ExpectedSM4 (high mass)
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A Test of the Fermiophobic Higgs Model Model tested: Assume SM-‐like behavior for the Higgs boson, except switch off all couplings to fermions. Decays for Hàbb, Hàττ, and Hàgg are highly suppressed. ggàH produc;on is neglibly small. WH, ZH, VBF produc;on cross sec;ons are as predicted by the SM HàWW, ZZ par;al widths are as predicted by the SM. Hàγγ is modified – loss of the fermion loop increases the decay rate. Hàγγ search is re-‐op;mized for this search because the pT spectrum of the H is harder in WH and ZH than for ggàH Branching ra;os recomputed using the modified decay widths.
Included channels: Hàγγ, HàWW, HàZZà4l
Observed exclusion: 100 < mH< 116 GeV/c2 Expected exclsuion: 100 < mH< 135 GeV/c2
T. Junk Tevatron Higgs Results
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M Tevatron Run II, Lint 10 fb-1
Fermiophobic Higgs combination
f
Expected w/o Higgs
Observed
Expected ±1 s.d.
Expected ±2 s.d.
FHM=1
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Constraining the Couplings of the Higgs Boson to Fermions and Gauge Bosons
We follow the procedures and nota;on of the LHC Higgs Cross Sec;on WG A. David et al., arXiv:1209.0040
The model: SM-‐like, but Hff couplings are scaled together by κf HWW coupling is scaled by κW HZZ coupling is scaled by κZ For some studies, we scale the HWW and HZZ couplings by κW=κZ=κV Standard Model: κf = κW = κZ = 1
T. Junk Tevatron Higgs Results 4/14/13
Step 1: Scale cross secMons for each process according to couplings
LO rela;ons, but mostly true at higher order (most QCD affects the colored ini;al-‐state par;cles. There is ggàWH at higher order, however.)
Constraining Couplings
! (gg!H ) =! SM (gg!H )(0.95" f2 + 0.05" f"V )
! (WH ) =! SM (WH )"V2
! (ZH ) =! SM (ZH )"V2
! (VBF) =! SM (VBF)"V2
A. David et al., LHCHXSWG-‐2012-‐001. arXiv:1209.0040
T. Junk Tevatron Higgs Results 4/14/13
Step 2: Recompute all Higgs boson decay branching raMos from scaled parMal widths α and β come from Spira et al., arXiv:hep-‐ph/9504378 α=1.28 β = -‐0.28
Constraining Couplings
!(H" gg) = !SM (H" gg)(0.95! f2 + 0.05! f!V )
!(H"W +W # ) = !SM (H"W +W # )!V2
!(H" bb ) = !SM (H" bb )! f2
!(H" " +" # ) = !SM (H" " +" # )! f2
!(H" cc ) = !SM (H" cc )! f2
!(H" ZZ ) = !SM (H" ZZ )!V2
!(H" ## ) = !SM (H" ## )$!V +%! f2
Br(H! XX) = "(H! XX)"i
i#
Other modes, like Hàμ+μ-‐ and HàZγ have very small widths
T. Junk Tevatron Higgs Results 4/14/13
Posterior Constraints on Coupling Scalings
• Uniform priors assumed. • Coupling scalings not shown are fixed to their SM values
Excess in the Hàγγ searches drives the asymmetry from posi;ve and nega;ve coupling scale factors
T. Junk Tevatron Higgs Results
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T. Junk Tevatron Higgs Results
WZ
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/4SM=
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floatingf
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Two-Dimensional Coupling Parameter Constraints
T. Junk Tevatron Higgs Results
V
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6Local maxima SM68% C.L. 95% C.L.
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=1WZ
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3 Local maxima SM68% C.L. 95% C.L.
-1 10 fb intTevatron Run II, L
floatingf
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T. Junk Tevatron Higgs Results
The Tevatron sees an excess of events consistent in all decay channels with the SM-‐Higgs-‐like par;cle observed at the LHC near mH=125 GeV/c2. Significance: 3.1σ at mH=125 GeV/c2. The Higgs boson does not look like that of the Fermophobic model or the SM with a fourth genera;on. Higgs boson couplings to W, Z, and fermions are consistent with SM predic;ons Extrac;ng coupling informa;on from the data requires full predic;ons of signal rates and shapes in all discriminants of all channels. Channels that contribute liile to the total SM sensi;vity can have outsized impacts on exo;c coupling scenario tests.
Summary
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